Show that the coefficient b2 for a quantum-mechanical Boltzmannian gas composed of ``spinless'' particles satisfies the following relations:
b2=J→∞lim{(2J+1)21b2S(J)}=J→∞lim{(2J+1)21b2A(J)}=21[b2S(0)+b2A(0)].
Obtain the value of b2, to fifth order in (r0/λ), by using the Beth–Uhlenbeck expressions (9.5.36, 37), and compare your result with the classical value of b2, namely −(2π/3)(r0/λ)3.